1992
DOI: 10.1103/physrevb.46.7682
|View full text |Cite
|
Sign up to set email alerts
|

Oscillator strength for intersubband transitions in strainedn-typeSixGe1

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
9
0

Year Published

1993
1993
2015
2015

Publication Types

Select...
4
2
1

Relationship

0
7

Authors

Journals

citations
Cited by 17 publications
(9 citation statements)
references
References 18 publications
0
9
0
Order By: Relevance
“…19 Sn 0.05 quantum cascade laser using intersubband transitions at L valleys of the conduction band which has a "clean" offset of 150 meV situated below other energy valleys ͑⌫ , X͒. The entire structure is strain-free because the lattice-matched Ge and Ge 0.76 Si 0.…”
mentioning
confidence: 99%
See 1 more Smart Citation
“…19 Sn 0.05 quantum cascade laser using intersubband transitions at L valleys of the conduction band which has a "clean" offset of 150 meV situated below other energy valleys ͑⌫ , X͒. The entire structure is strain-free because the lattice-matched Ge and Ge 0.76 Si 0.…”
mentioning
confidence: 99%
“…The entire structure is strain-free because the lattice-matched Ge and Ge 0.76 Si 0. 19 Sn 0.05 layers are to be grown on a relaxed Ge buffer layer on a Si substrate. Longer lifetimes due to the weaker scattering of nonpolar optical phonons reduce the threshold current and potentially lead to room temperature operation.…”
mentioning
confidence: 99%
“…where p is the momentum operator. 12 Using the aforementioned value of m zz and 1/m xz =1/͑3m t ͒ −1/͑3m l ͒ =1/͑0.26m 0 ͒, a non-negligible TEto-TM gain ratio g TE / g TM = ͑m zz / m xz ͒ 2 = 0.21 is obtained. 12,13 To model intravalley deformation-potential scattering, the following expressions can be used for the transition rates between subbands ͉i͘ and ͉f͘ due to emission ͑upper sign͒ and absorption ͑lower sign͒ of optical and acoustic phonons, respectively: 15…”
Section: ͑1͒mentioning
confidence: 99%
“…1, the constant-energy ellipsoids around the L-valley minima are tilted with respect to the ͑001͒ growth direction ͑z͒, giving rise to an inverse effective-mass tensor with both diagonal and off-diagonal nonzero terms. The relevant perpendicular effective mass is the diagonal term m zz , 12 which is related to the principal L-valley effective masses m l and m t according to 13 1/m zz =2/͑3m t ͒ +1/͑3m l ͒. Using m t = 0.08m 0 and m l = 1.59m 0 for Ge, 7 we obtain m zz = 0.12m 0 , which is about three times smaller than the mass of the heavy holes used in the SiGe ISB emitters of Refs.…”
mentioning
confidence: 99%
See 1 more Smart Citation